lecture 1 - basic physics - universiteit utrecht 1 - basic physics.… · when two objects come...

Lecture I: Basic Physics

1

2Lecture I: Basic Physics

• Suppose object position 𝑝" and constant velocity �⃗�. At time 𝑡:• 𝑝" 𝑡 + ∆𝑡 = 𝑝" 𝑡 + �⃗�∆𝑡• ∆𝑝" = 𝑝" 𝑡 + ∆𝑡 − 𝑝" 𝑡 = �⃗�∆𝑡• If 𝑝" 0 = 𝑃, then 𝑝" 𝑡 = 𝑃 + �⃗�𝑡

• …�⃗� is never constant in practice• A function of time�⃗�(𝑡), so 𝑝" 𝑡 𝑠 = 𝑃 + ∫ �⃗� 𝑡 𝑑𝑡

23

• Position is integrated in time.• Velocity units: 4 256⁄

Velocity


• Instantaneous change in velocity: �⃗� = 9: 9;< .• Constant acceleration: ∆�⃗� = �⃗�∆𝑡.• Otherwise, integrate:𝑣 𝑠 = V + ∫ 𝑎 𝑡 𝑑𝑡23 .

• Note vector quantities!• Position: trajectory of a point.• Velocity: tangent to trajectory curve.

• Speed: absolute value of velocity.• Acceleration: the change in the tangent.

Acceleration


• Using coordinates, our vector quantities are relative to the chosen axis system.• They are viewpoint dependent.

• The derivation/integration relations are invariant!

Relative Quantities


• Acceleration is induced by a force.

• Direction of force = direction of associated acceleration.

• Net force (and net acceleration): the sum of all acting forces.

Forces


• In the late 17th century, Sir Isaac Newton described three laws that govern all motion on Earth.

• ...ultimately, an approximation• Small scale: quantum mechanics.• Big scale: theories of relativity.

Newton’s laws of motion


• Sum of forces on an object is null ó there is no change in the motion

• With zero force sum:• An object at rest stays at rest.• A moving object continues to in the same velocity.

1st Law of Motion

If 𝐹?5; = 0, there is no change in motion


• Each force induces a co-directional acceleration in linear to the mass of the object:

• Consequently:• More force ó faster speed-up.• Same force ó lighter objects accelerate faster than

heavy objects.

2nd Law of Motion

�⃗�?5; = 𝑚 ∗ �⃗�𝑚 is the mass and 𝑎 the acceleration


• Forces have consequences:

• All forces are actually interactions between bodies!

3rd Law of Motion

When two objects come into contact, they exert equal and opposite forces upon each other.

What happens here?


• Newton’s Law of Gravitation: the gravitation force between two masses 𝐴 and 𝐵 is:

�⃗�D = �⃗�E→G = −�⃗�G→E = 𝐺𝑚E𝑚G𝑟J

𝑢EG𝐺: gravitational constant 6.673×10STT[𝑚V𝑘𝑔ST𝑠SJ].𝑟: the distance.

𝑢EG =Y⃗ZSY⃗[

Y⃗ZSY⃗[< : the unit direction between the

locations.

Gravity


• By applying Newton’s 2nd law to an object with mass 𝑚 on the surface of the Earth, we obtain:

�⃗�?5; = �⃗�D = 𝑚 ∗ �⃗�

𝐺 4∗4\]^_`a\]^_`b

= 𝑚 ∗ 𝑎

𝐺 4\]^_`a\]^_`b

= 𝑎

𝑎 = 6.673×10STT c.de×T3bf

g.Vhh×T3i b= 9.81𝑚/𝑠J

Gravity on Earth

Mass of object is canceled out!

http://lannyland.blogspot.co.at/2012/12/10-famous-thought-experiments-that-just.html


• On Earth at altitude ℎ: 𝑎 = 𝐺 4\]^_`a\]^_`no b

• On the Moon• 𝑚4""? = 7.35×10JJ𝑘𝑔• 𝑟4""? = 1738𝑘𝑚• 𝑔4""? = 1.62𝑚/𝑠J

• On Mars• 𝑚4ra2 = 6.42×10JV𝑘𝑔• 𝑟4ra2 = 3403𝑘𝑚• 𝑔4ra2 = 3.69𝑚/𝑠J

Gravity on Other Planets


• Weight ó gravitational force

𝑊 = 𝑚 ∗ �⃗�• We weigh differently on the moon (but have the

same mass…)

• Force units: 𝑘𝑔 u 4256b

.• Denoted as Newtons (𝑁)

Weight


• Force acting as a reaction to contact.• Direction is normal to the surface of contact.• Magnitude enough to cancel the weight applied on the

plane.

• Here, 𝐹w = 𝑊 cos(𝛼) = 𝑚𝑔 cos(𝛼)• Related to collision handling (more later).• Object slides down plane with remaining force:𝑊sin(𝛼).

Normal force


• Can the object stay in total equilibrium?• An extra tangential friction force must cancel 𝑊sin(𝛼).

• Ability to resist movement.• Static friction keeps an object on a surface from moving.• Kinetic friction slows down an object in contact.

Friction


• Static friction: a threshold force. • object will not move unless tangential force is stronger.

• Kinetic friction: when the object is moving.

• Depends on the materials in contact.• smoother ó less friction.

• Coefficient of friction 𝜇 determines friction forces:• Static friction: 𝐹2 = 𝜇2𝐹w• Kinetic friction: 𝐹 = 𝜇𝐹w

Friction


• The kinetic coefficient of friction is always smaller than the static friction.

• If the tangential force is larger than the static friction, the object moves.

• If the object moves while in contact, the kinetic friction is applied to the object.

Friction


Surface Friction Static (𝝁𝒔) Kinetic (𝝁𝒌)

Steel on steel (dry) 0.6 0.4

Steel on steel (greasy) 0.1 0.05

Teflon on steel 0.041 0.04

Brake lining on cast iron 0.4 0.3

Rubber on concrete (dry) 1.0 0.9

Rubber on concrete (wet) 0.30 0.25

Metal on ice 0.022 0.02

Steel on steel 0.74 0.57

Aluminum on steel 0.61 0.47

Copper on steel 0.53 0.36

Nickel on nickel 1.1 0.53

Glass on glass 0.94 0.40

Copper on glass 0.68 0.53

Friction


• An object moving in a fluid (air is a fluid) is slowed down by this fluid.

• This is called fluid resistance or drag and depends on several parameters, e.g.:• High velocity ó larger resistance.• More surface area ó larger resistance (“bad

aerodynamics”).

Fluid resistance


• At high velocity, the drag force 𝐹oDo is quadraticto the relative velocity 𝑣of the object:

𝐹`` = −TJ∗ 𝜌 ∗ 𝑣J ∗ 𝐶9 ∗ 𝐴

• 𝜌 is the density of the fluid (1.204 for air at 20℃)• 𝐶9 is the drag coefficient (depends on the shape of

the object).• 𝐴 is the reference area (area of the projection of

the exposed shape).

Fluid resistance


• At low velocity, the drag force is approximately linearly proportional to the velocity

𝐹 ≈ −𝑏 ∗ 𝑣

where 𝑏 depends on the properties of the fluid and the shape of the object.• High/low velocity threshold is defined by Reynolds

Number (Re).

Fluid resistance


• Develops when an object is immersed in a fluid.

• A function of the volume of the object 𝑉 and the density of the fluid 𝜌:

𝐹G = 𝜌 ∗ 𝑔 ∗ 𝑉

• Considers the difference of pressure above and below the immersed object.

• Directed straight up, counteracting the weight.

Buoyancy1.14


• React according to Hook’s Law on extension and compression, i.e. on the relative displacement.

• The relative length 𝑙 to the rest length 𝑙3determines the applied force:

𝐹 = −𝐾 𝑙 − 𝑙3

• 𝐾 is the spring constant (in 𝑁/𝑚).

Springs


• Without interference, objects may oscillate infinitely.

• Dampers slow down the oscillation between objects 𝐴 and 𝐵 connected by a spring.

• Opposite to the relative speed between the two objects:

𝐹 = −𝐶(𝑣E − 𝑣G)• 𝐶 is the damping coefficient. • Resulting force applied on 𝐴 (opposite on 𝐵).

• Similar to friction or drag at low velocity!

Dampers


• To get acceleration: sum forces and divide by mass:

�⃗�?5; =�⃗� = 𝑚 ∗ �⃗�

• Forces add up linearly as vectors. The Free Body Diagram includes:• Object shape: center of mass, contact points.• Applied forces: direction, magnitude, and point of

application.

Free-Body Diagram

https://www2.southeastern.edu/Academics/Faculty/rallain/plab193/files/a8312fbf3bde4804309096169ad22bd5-46.html


• A force �⃗� does work 𝑊 (in 𝐽𝑜𝑢𝑙𝑒 = 𝑁 u 𝑚), if it achieves a displacement ∆𝑝 in the direction of the displacement:

𝑊 = �⃗� u ∆𝑝

• Note dot product between vectors.• Scalar quantity.

Work

𝐹

𝐹 cos𝛼𝛼


• The kinetic energy 𝐸 is the energy of an object in velocity:

𝐸 =12𝑚 𝑣 J

• The faster the object is moving, the more energy it has.• The energy is a scalar (relative to speed, regardless of

direction).• Unit is also Joule:

𝑘𝑔(𝑚/𝑠𝑒𝑐)J= 𝑘𝑔 ∗ 4256b 𝑚 = 𝑁 ∗ 𝑚 = 𝐽

Kinetic energy


• The Work-Energy theorem: net work ó change in kinetic energy:

𝑊 = ∆𝐸 = 𝐸(𝑡 + ∆𝑡) − 𝐸(𝑡)i.e.

�⃗� u ∆𝑝 =12𝑚 𝑣(𝑡 + ∆𝑡)J − 𝑣(𝑡)J

• Very similar to Newton’s second law...

Work-Energy theorem1.15


• (Gravitational) Potential energy is the energy ‘stored’ in an object due to relative height difference.• The amount of work that would be done if we were to set

it free.𝐸 = 𝑚 u 𝑔 u ℎ

• Simple product of the weight 𝑊 = 𝑚 u 𝑔 and height ℎ.• Also measured in Joules (as here 𝑘𝑔 u 4256b u 𝑚).

• Other potential energies exist (like a compressed spring).

Potential energy


• Law of conservation: in a closed system, energy cannot be created or destroyed.• Energy may switch form.• May transfer between objects.• Classical example: falling trades potential and kinetic

energies.

𝐸(𝑡 + ∆𝑡) + 𝐸(𝑡 + ∆𝑡) = 𝐸(𝑡) + 𝐸(𝑡)i.e.

12𝑚𝑣(𝑡 + ∆𝑡)J + 𝑚𝑔ℎ 𝑡 + ∆𝑡 =

12𝑚𝑣(𝑡)J + 𝑚𝑔ℎ 𝑡

Conservation of mechanical energy


• A roller-coaster cart at the top of the first hill• Much potential energy but only a little kinetic energy.• Going down the drop: losing height, picking up speed.• At the bottom: almost all potential energy switched to

kinetic, cart is at its maximum speed.

Conservation: Example


• External forces are usually applied:• Friction and air resistance.• Where does the “reduced” energy go?• Converted into heat and air displacements (sound

waves, wind).• We compensate by adding an extra term 𝐸 to the

conservation equation:𝐸 𝑡 + ∆𝑡 + 𝐸 𝑡 + ∆𝑡 + 𝐸 = 𝐸 𝑡 + 𝐸 𝑡

• if 𝐸 > 0, some energy is ‘lost’.

Conservation of Mechanical Energy

https://i.ytimg.com/vi/anb2c4Rm27E/maxresdefault.jpg


• The linear momentum 𝑝:the mass of an object multiplied by its velocity:

�⃗� = 𝑚 ∗ 𝑣

• Heavier object/higher velocity ó more momentum (more difficult to stop).

• unit is 𝑘𝑔 u 4 256⁄ .

• Vector quantity (velocity).

Momentum


• A change of momentum:𝚥 = ∆𝑝

• Compare:• Impulse is change in momentum.• Work is change in energy.

• Unit is also 𝑘𝑔 u 4256

(like momentum).

• Impulse ó force integrated over time:

Impulse

𝐽 = �⃗�𝑑𝑡;

3= 𝑚 �⃗�𝑑𝑡

;

3= 𝑚Δ�⃗�.

lecture 1 - basic physics - universiteit utrecht 1 - basic physics.… · when two objects come...

Documents